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United States Patent |
5,686,177
|
Yamanaka
,   et al.
|
November 11, 1997
|
Magnetic recording medium
Abstract
A magnetic recording medium having an improved S/N is provided by using a
ferromagnetic metal thin film having a mean value of a fluctuation field
of magnetic viscosithy measured at 25.degree. C. in a region in which an
applied magnetic field strength is 0.8 to 1.2 times as large as a
remanence coercivity, of between 15 Oersteads and 30 Oersteads, and
preferably a coercivity of between 700 Oersteads and 2000 Oersteads.
Inventors:
|
Yamanaka; Kazusuke (Kanagawa-ken, JP);
Kusada; Hideo (Ibaraki-ken, JP);
Okuwaki; Toyoji (Tokyo, JP)
|
Assignee:
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Hitachi, Ltd. (Tokyo, JP)
|
Appl. No.:
|
290259 |
Filed:
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August 15, 1994 |
Foreign Application Priority Data
Current U.S. Class: |
428/332; 360/110; 428/827 |
Intern'l Class: |
G11B 005/66; G11B 021/00; H01F 010/16 |
Field of Search: |
428/694 T,694 TM,694 TS,332,65.3
204/192.2
360/110
|
References Cited
U.S. Patent Documents
4511635 | Apr., 1985 | Nagao et al. | 428/694.
|
4520076 | May., 1985 | Saito et al. | 428/694.
|
4521481 | Jun., 1985 | Nagao et al. | 428/336.
|
4663193 | May., 1987 | Endo et al. | 427/129.
|
5370928 | Dec., 1994 | Funabashi et al. | 428/336.
|
Foreign Patent Documents |
415335A2 | Mar., 1991 | EP.
| |
488377A2 | Jun., 1992 | EP.
| |
530379A1 | Mar., 1993 | EP.
| |
Other References
Journal of Physics, F Metal Physics, vol. 14, pp. L155-L159 (1984) no
month.
Journal of Magnetism and Magnetic Materials, vol. 127, pp. 233-240 (1993)
no month.
|
Primary Examiner: Zimmerman; John J.
Assistant Examiner: LaVilla; Michael
Attorney, Agent or Firm: Kenyon & Kenyon
Claims
What is claimed is:
1. A magnetic recording medium comprising:
a magnetic layer having at least one ferromagnetic cobalt-based thin film,
the fluctuation field of said layer of a predetermined magnetic viscosity
measured at 25.degree. C. and at a magnetic field equal to a predetermined
remanence coercivity being between 15 Oersteads and 30 Oersteads;
the magnetic layer having a coercivity of between 700 Oerstead and 2000
Oersteads; and
the thickness of said magnetic layer being between 0.1 and 0.18 .mu.m.
2. A magnetic recording medium according to claim 1 wherein said
ferromagnetic thin film is a cobalt based thin film selected from Co--O,
Co--Ni, Co--Cr, Co--Mo, Co--Ta, Co--Ni--Cr and Co--Ni--O.
3. A magnetic recording medium according to claim 1 wherein said magnetic
recording medium comprises a magnetic tape.
4. A magnetic recording medium comprising:
a magnetic layer having at least one ferromagnetic cobalt-based thin film,
the fluctuation field of said layer of a predetermined magnetic viscosity
measured at 25.degree. C. and at magnetic field equal to a predetermined
remanence coercivity being between 20 Oersteads and 30 Oersteads;
the magnetic layer having a coercivity of between 700 Oerstead and 2000
Oersteads; and
the thickness of said magnetic layer being between 0.1 and 0.18 .mu.m.
5. A magnetic recording medium according to claim 4 wherein said
ferromagnetic thin film is a cobalt based thin film selected from Co--O,
Co--Ni, Co--Cr, Co--Mo, Co--Ta, Co--Ni--Cr and Co--Ni--O.
6. A magnetic recording medium according to claim 4 wherein said magnetic
recording medium comprises a magnetic tape.
7. A magnetic recording apparatus comprising:
a magnetic head having a ferromagnetic thin film in a portion of a magnetic
pole thereof; and
a magnetic recording medium having a ferromagnetic cobalt-based thin film
as a magnetic layer;
said thin film of said magnetic recording medium having a mean value of a
fluctuation field of a predetermined magnetic viscosity at 25.degree. C.
and a magnetic field equal to a predetermined remanence coercivity which
is between 15 Oersteads and 30 Oersteads;
said magnetic layer of said magnetic recording medium having a coercivity
of between 700 Oersteads and 2,000 Oersteads; and
said magnetic layer of said magnetic recording medium having a thickness of
between 0.1 and 0.18 .mu.m.
8. A magnetic recording apparatus comprising:
a magnetic head having a ferromagnetic thin film in a portion of a magnetic
pole thereof; and
a magnetic recording medium having a ferromagnetic cobalt-based thin film
as a magnetic layer;
said thin film of said magnetic recording medium having a mean value of a
fluctuation field of a predetermined magnetic viscosity at 25.degree. C.
and at an applied magnetic field equal to a predetermined remanence
coercivity which is between 20 Oersteads and 30 Oersteads;
said magnetic layer of said magnetic recording medium having a coercivity
of between 700 Oersteads and 2,000 Oersteads; and
said magnetic layer of said magnetic recording medium having a thickness of
between 0.1 and 0.18 .mu.m.
Description
BACKGROUND OF THE INVENTION
The present invention relates to a ferromagnetic metal thin film magnetic
recording medium and a magnetic recording and reproducing apparatus, and
more particularly to a magnetic recording medium having an excellent
electromagnetic transducing property and a bulk magnetic recording and
reproducing apparatus.
The fineness of magnetic particles in a coating type medium and crystal
grains in a thin film medium is essential to improve a recording density
and attain a high output power and low noise in a magnetic recording
medium. For example, in a medium which uses iron particles studied in the
past, the fineness has been increased such that a high performance tape
such as Hi-8 which uses fine particles having a cylinder major axis length
of approximately 0.2 .mu.m and an cylinder diameter of approximately 0.03
.mu.m is presently put into practice.
Even if the magnetic particles or the crystal grains of the magnetic medium
are fine, a plurality of particles or grains may have the magnetization
thereof reversed in group when the magnetic particles are in a clustered
agglomerate or an interaction among the crystal grains is strong. When a
unit of magnetization reversal increases as a plurality of particles or
grains have the magnetization thereof reversed in group, a noise in a
reproducing mode increases. This is a serious barrier to high density
recording.
The size of the unit of magnetization reversal relates to a magnetic
viscosity. Namely, it has been considered that the larger a fluctuation
field is, the smaller is the unit of magnetization reversal.
The definition and a measuring method of the fluctuation field of the
magnetic viscosity are described in Journal of Physics, F Metal Physics,
Vol.14, pages L155.about.L159 (1984).
More detailed measurement method is disclosed in Journal of Magneticism and
Magnetic Material, Vol. 127, pages 233.about.240 (1993).
SUMMARY OF THE INVENTION
It is an object of the present invention to provide a magnetic recording
medium and a magnetic recording and reproducing apparatus which reduce a
noise in the reproducing mode and which are suitable for high density
recording.
In order to solve the above problems, the present invention aims to
minimize the unit of magnetization reversal as much as possible. As a
reference to determine the size of the unit of magnetization reversal, the
fluctuation field of the magnetic viscosity is used. It has been found
that a ferromagnetic thin film having a mean fluctuation field the
magnetic viscosity of 15 Oersteads to 30 Oersteads at 25.degree. C. in a
region of an applied magnetic field strength which is 0.8 to 1.2 times as
large as a remanence coercivity, and having a coercivity of 700 Oersteads
to 2000 Oersteads, with a thickness of the magnetic film being 0.1 .mu.m
to 0.18 .mu.m, can significantly reduce a noise level. It has also been
found that preferable ferromagnetic thin films are those containing cobalt
such as Co--O, Co--Ni, Co--Cr, Co--Mo, Co--Ta, Co--Ni--Cr or Co--Ni--O.
Since the magnetic recording medium of the present invention can reduce the
cluster size in the magnetization reversal, a noise level can be lowered
and an S/N ratio can be raised. By combining it with a magnetic head which
uses a metal magnetic film as a portion of a magnetic pole, an to
significantly improved recording characteristic of the medium is derived
and a bulk recording and reproducing apparatus may be provided.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 shows a sectional view of a magnetic recording medium in accordance
with one embodiment of the present invention,
FIG. 2 shows a characteristic chart of a relationship between a coercivity
and a fluctuation field, and an S/N ratio for a magnetic layer having a
total film thickness of 0.01 .mu.m,
FIG. 3 shows a characteristic chart of a relationship between a coercivity
and a fluctuation field and an S/N ratio for a magnetic layer having a
total film thickness of 0.14 .mu.m; and
FIG. 4 shows a characteristic chart of a relationship between a coercivity
and a fluctuation field, and an S/N ratio for a magnetic layer having a
total film thickness of 0.18 .mu.m.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Referring to the accompanying drawings, the present invention is explained.
FIG. 1 shows an enlarged sectional view of a magnetic recording medium of
the present invention. In FIG. 1, numeral 1 denotes a polymer film such as
polyethylene terephthalate, polyethylene-2, 6-naphthalate, polyether ether
ketone, polyphenylene sulfide or polyether sulfonamide, with a surface
having fine particles homogeneously dispersed and coated or dispersed and
coated in a discontinuous film arranged thereon as required. Numerals 2
and 3 denote a cobalt-based ferromagnetic thin film such as Co--O, Co--Ni,
Co--Cr, Co--Mo, Co--Ta, Co--Ni--Cr or Co--Ni--O. In the present
embodiment, it is a two-layer structure of the magnetic layers 2 and 3.
Numeral 4 denotes a protective lubricant layer which may be a carbon film,
a metal oxide film, a plasma polymerized film, fatty acid, perfluorocarbon
carboxylic acid or perfluoropolyether. Numeral 5 denotes a back-coated
layer having resin and filler mixedly dispersed. The magnetic layer 2 is
preferably a ferromagnetic thin film which exhibits a mean fluctuation
field at 25.degree. C. of 15 Oersteads to 30 Oersteads in a region in
which an applied magnetic field strength is 0.8 to 1.2 times as large as a
remanence coercivity, and a coercivity of 700 Oersteads to 2000 Oersteads
with an overall thickness of the magnetic layer being 0.1 .mu.m to 0.18
.mu.m. It is also preferable that the ferromagnetic thin film is a cobalt
based magnetic alloy thin film which contains at least one element
selected from a group consisting of O, Ni, Cr, Mo, V, Ti, Zr, Pt, Hf and
Si.
In the present embodiment, the magnetic tape is discussed although the
present invention is effective to other magnetic recording material such
as a magnetic disk. A prior art medium will be described as a comparative
example and examples of the present invention will also be described.
›Comparative Example!
A ferromagnetic thin film was formed on a polyethylene terephthalate film
in a prior art method. Co--Ni (Ni content: 20% by weight) was obliquely
evaporated on a polyethylene terephthalate film having a thickness of 10
.mu.m in vacuum containing a small amount of oxygen to form a magnetic
layer of acicular fine particles consisting of Co--Ni--O. An oxygen flow
rate was 300 cc/min. Thicknesses of the magnetic films were 0.1 .mu.m
(tape A), 0.14 .mu.m (tape B) and 0.18 .mu.m (tape C). Coercivities
measured while a magnetic field was applied longitudinally of the tapes
were 1000 Oersteads, 1300 Oersteads and 1350 Oersteads, respectively.
Fluctuation fields of magnetic viscosity of those tapes were measured at
25.degree. C. with a magnetic field application time of 0 to 30 minutes.
Mean values of the fluctuation field in a region in which an applied
magnetic field strength was 0.8 to 1.2 times as large as a remanence
coercivity were 14 Oersteads for the tape A, 12 Oersteads for the tape B
and 10 Oersteads for the tape C. S/N when recorded at 7 MHz were +0.2 dB
for the tape B and +0.1 dB for the tape C assuming that it was 0 dB for
the tape A.
›EXAMPLE 1!
In the present example, the magnetic layer is of single or double layer
structure having a total thickness of 0.1 .mu.m. For the double layer
structure, a very thin non-magnetic oxide layer was interposed between the
magnetic layers. Like the comparative example, Co--Ni (Ni content: 20% by
weight) was obliquely evaporated on a polyethylene terephthalate film in
vacuum containing a small amount of oxygen to form a magnetic layer of
acicular fine particles primarily consisting of Co--Ni--O. The oxygen flow
rate was changed from 100 cc/min to 500 cc/min and the temperature of the
polyethylene terephthalate film base during the evaporation was changed
from 5.degree. C. to 50.degree. C. to form 30 tapes in total. Of those,
ten were of single magnetic layer structure and the remaining twenty were
of double layer structure of magnetic layers of 0.05 .mu.m thickness with
a non-magnetic oxide layer being interposed. The coercivities of the ten
tapes of the single magnetic layer structure distributed from 950
Oersteads to 1650 Oersteads. The mean values of the fluctuation field
(measured at 25.degree. C.) in the region in which the applied magnetic
field strength was 0.8 to 1.2 times as large as the remanence coercivity
distributed from 10.5 Oersteads to 14.8 Oersteads. The S/N ratios recorded
at 7 MHz distributed from -2.3 dB to +0.3 dB assuming the S/N of the tape
A of the comparative example was 0 dB. Thus, when the magnetic layer was
of single layer structure, significant improvement of the S/N ratio was
not attained even if the oxygen flow rate and the temperature of the
polyethylene terephthalate film base were changed.
On the other hand, the coercivities of the 20 tapes of the double layer
structure of the magnetic layers of 0.05 .mu.m thick with the interposed
non-magnetic oxide layer distributed from 600 Oersteads to 1350 Oersteads.
The mean values of the fluctuation fields measured at 25.degree. C. in the
region in which the applied magnetic field strength was 0.8 to 1.2 times
as large as the remanence coercivity distributed from 16.6 Oersteads to
35.8 Oersteads. The S/N ratios in the recording at 7 MHz distributed from
-3.2 dB to +1.8 dB assuming that the S/N of the tape A of the comparative
example was 0 dB. Based on those data, assuming that the S/N of the tape A
is 0 dB, the region which showed the improvement of S/N of no smaller than
+1.0 dB is plotted in FIG. 2 with an ordinate representing a coercivity Hc
and an abscissa representing a mean value of fluctuation field measured at
25.degree. C. in the region in which the applied magnetic field H is 0.8
to 1.2 times as large as a remanence coercivity Hr. The measurement time
of the magnetic viscosity was 0 to 30 minutes. In FIG. 2, white circles
indicate the improvement of the S/N of no smaller than 1.0 dB over that of
the tape A, and black dots indicate the improvement under 1.0 dB. As seen
form FIG. 2, the S/N ratios are improved by no smaller than +1.0 dB when
the coercivity is no smaller than 700 Oersteads and the mean value of the
fluctuation field measured at 25.degree. C. in the region in which the
applied magnetic field is 0.8 to 1.2 times as large as the remanence
coercivity is no smaller than 15 Oersteads.
When the total film thickness was no larger than 0.08 .mu.m, the
improvement of the S/N of no smaller than +1.0 dB was not attained whether
the magnetic layer was of single layer structure or double layer
structure.
›EXAMPLE 2!
In the present example, the magnetic layer is of single or double layer
structure having a total film thickness of 0.14 .mu.m. For the double
layer structure, a non-magnetic oxide was interposed between the magnetic
layers. Like the comparative example, Co--Ni was obliquely evaporated on a
polyethylene terephthalate film of 10 .mu.m thick in vacuum containing a
small amount of oxygen to form a magnetic layer of acicular fine particles
primarily consisting of Co--Ni--O. The Ni content in the Co--Ni alloy was
13 to 25% by weight. Total of 40 tapes were manufactured while the oxygen
flow rate was changed from 100 cc/min to 500 cc/min and the temperature of
the polyethylene terephthalate film base during the evaporation was
changed from 5.degree. C. to 50.degree. C. Of those, 20 magnetic layers
were of single layer structure and the remaining 20 were of double layer
structure of the magnetic layers of 0.07 .mu.m thick with the interposed
non-magnetic oxide layer. The coercivities of the 20 tapes of the single
magnetic layer structure distributed from 940 Oersteads to 1830 Oersteads.
The mean values of the fluctuation field measured at 25.degree. C. in the
region in which the applied magnetic field strength was 0.8 to 1.2 times
as large as the remanence coercivity distributed from 8.4 Oersteads to
12.6 Oersteads. The S/N ratios when recorded at 7 MHz distributed from
-1.8 dB to +0.4 dB assuming that the S/N of the tape A of the comparative
example was 0 dB. Thus, for the magnetic layer of the single layer
structure, the significant improvement of the S/N was not attained even if
the oxygen flow rate and the temperature of the polyethylene terephthalate
film base were changed.
On the other hand, the coercivities of the 20 tapes of the double layer
structure of the magnetic layer of 0.07 .mu.m with the interposed
non-magnetic oxide layer distributed from 680 Oersteads to 1470 Oersteads.
The mean values of fluctuation field measured at 25.degree. C. in region
in which the applied magnetic field strength was 0.8 to 1.2 times as large
as the remanence coercivity distributed from 14.6 Oersteads to 30.4
Oersteads. Further, the S/N ratios when recorded at 7 MHz distributed from
-1.4 dB to +2.1 dB assuming that the S/N of the tape A of the comparative
example was 0 dB. Based on those data, assuming that the S/N of the tape A
is 0 dB, the region in which the S/N was improved by no smaller than +1.0
dB is plotted in FIG. 3 with an ordinate representing a coercivity Hc and
an abscissa representing a mean value of fluctuation field in the region
in which the applied magnetic field strength is 0.8 to 1.2 times as large
as the remanence coercivity Hr. As seen from FIG. 3, the S/N was improved
by no smaller than +1.0 dB when the coercive force was no smaller than 700
Oersteads and the mean value of the fluctuation field measured at
25.degree. C. in the region in which the applied magnetic field strength
was 0.8 times as large as the remanence coercivity was between 15
Oersteads and 30 Oersteads.
›EXAMPLE 3!
In the present example, the magnetic layer is of single or double layer
structure having a total film thickness of 0.18 .mu.m. For the double
layer structure, a non-magnetic oxide was interposed between the magnetic
layers. Like the comparative example, Co--Ni was obliquely evaporated on a
polyethylene terephthalate film of 10 .mu.m thick in vacuum containing a
small amount oxygen to form a magnetic layer of acicular fine particles
primarily consisting of Co--Ni--O. The Ni content in the Co--Ni alloy was
13 to 25% by weight. Total of 40 tapes were manufactured while the oxygen
flow rate was changed from 100 cc/min to 500 cc/min and the temperature of
the polyethylene terephthalate film base during the evaporation was
changed from 5.degree. C. to 50.degree. C. Of those, 20 magnetic layers
were of single layer structure and the remaining 20 were of double layer
structure of the magnetic layers of 0.09 .mu.m thick with the interposed
non-magnetic oxide layer. The coercivities of the 20 tapes of the single
magnetic layer structure distributed from 980 Oersteads to 1860 Oersteads.
The mean values of the fluctuation field measured at 25.degree. C. in the
region in which the applied magnetic field strength was 0.8 to 1.2 times
as large as the remanence coercivity distributed from 7.3 Oersteads to
12.1 Oersteads. The S/N ratios when recorded at 7 MHz distributed from
-2.1 dB to +0.2 dB assuming that the S/N of the tape A of the comparative
example was 0 dB. Thus, for the magnetic layer of the single layer
structure, the significant improvement of the S/N was not attained even if
the oxygen flow rate and the temperature of the polyethylene terephthalate
film base were changed.
On the other hand, the coercivities of the 20 tapes of the double layer
stricture of the magnetic layer of 0.09 .mu.m with the interposed
non-magnetic oxide layer distributed from 690 Oersteads to 1860 Oersteads.
The mean values of fluctuation field measured at 25.degree. C. in the
region in which the applied magnetic field strength was 0.8 to 1.2 times
as large as the remanence coercivity distributed from 12.6 Oersteads to
26.1 Oersteads. Further, the S/N ratios when recorded at 7 MHz distributed
from -1.0 dB to +1.2 dB assuming that the S/N of the tape A of the
comparative example wads 0 dB. Based on those data, assuming that the S/n
of the tape A is 0 dB, the region in which the S/N was improved by no
smaller than +1.0 dB is plotted in FIG. 4 with an ordinate representing a
coercivity Hc and an abscissa representing a mean value of fluctuation
field in the region in which the applied magnetic field strength is 0.8 to
1.2 times as large as the remanence coercivity Hr. As seen from FIG. 4,
the S/N was improved by no smaller than +1.0 dB when the coercive force
was no smaller than 700 Oersteads and the mean value of the fluctuation
field measured at 25.degree. C. in the region in which the applied
magnetic field strength was 0.8 times as large as the remanence coercivity
was between 15 Oersteads and 30 Oersteads.
Further, when the mean value of fluctuation field was no smaller than 20
Oersteads, the improvement of over +1.5 dB was attained.
In the examples, the fluctuation field is the mean value measured at
25.degree. C. in the region in which the applied magnetic field strength
is 0.8 to 1.2 times as Furthermore, it is has been improved that the mean
value of the fluctuation field, measured at 25.degree. C., between the
limits of 0.8 and 1.2 times the remanence coercivity is equal to the value
of the fluctuation field measured at a magnetic field strength equal to
the remanence coercivity.
When the total film thickness was no smaller than 0.18 .mu.m, the
improvement of S/N by no smaller than +1.0 dB was not attained whether the
magnetic layer was of single layer structure or double layer structure.
In the examples, the Co--Ni alloy is used as the ferromagnetic thin film
although it will be readily understood that the present invention is also
effective when a thin film containing cobalt such as Co--O, Co--Cr,
Co--Mo, Co--Ta, or Co--N--Cr is used. A similar effect is obtained when
three or more magnetic layers are used.
In accordance with the present invention, when the ferromagnetic thin film
is used as the magnetic layer, the coercivity thereof is selected to be no
smaller than 700 Oersteads, and the mean value of the fluctuation field
measured at 25.degree. C. in the region in which the applied magnetic
field strength is 0.8 to 1.2 times as large as the remanence coercivity is
selected between 15 Oersteads and 30 Oersteads, the S/N of the medium can
be significantly improved and the high density recording is attained.
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